Increasing mass, decreasing force?

As a neutron star collapses further and neutron degeneracy pressure causes
neutrons to increase in mass (by virtue of high speeds),
if that mass increase weakens the force of gravity it could stop
a singularity from forming.Is there any evidence that particles with large mass
increases due to high speed experience a weaker gravitational field?

As the neutron star collapses, both the density and pressure will increase. Both of these will increase the gravitational field, because both the density and the pressure contribute to the stress-energy tensor in a manner that will increase the Einstein curvature.

It's best not to talk about "increases in mass" of neutrons. To say that the mass increases as written is incorrect - saying that the "realtivsitc mass increases" would not be wrong, but the usage is debatable (we have an off-and-on debate about that far too often already, let's not start another one).

The reason I asked is because in the Bohr model of hydrogen a 1s electron orbits faster than a 2s electron and so then 1s electron would have more relativistic mass.
If this is associated with a weaker force - in this case a weaker electric force than expected between the proton and electron - then it might account for the lamb shift. I was just wondering if speed could weaken gravity.Those singularities have to be stopped from forming - they don't make sense to me.

The reason I asked is because in the Bohr model of hydrogen a 1s electron orbits faster than a 2s electron and so then 1s electron would have more relativistic mass.

The Bohr model has long been discarded - try something a little more modern?

In any event, if you look hard enough, you can find the so-called "relativistic correction" calculation using perturbation theory. The first-order correction is larger than the Lamb shift by about a factor of the fine structure constant. The second and higher order corrections are insignificant.

You can also get an 'exact' solution from the Dirac equation for the electron which fully accounts for spin-orbit and relativistic structure. It doesn't predict a Lamb shift.

If this is associated with a weaker force - in this case a weaker electric force than expected between the proton and electron - then it might account for the lamb shift

I think I'll stick with the account provided by QED for now

I was just wondering if speed could weaken gravity.Those singularities have to be stopped from forming - they don't make sense to me.

As the neutron star collapses, both the density and pressure will increase. Both of these will increase the gravitational field, because both the density and the pressure contribute to the stress-energy tensor in a manner that will increase the Einstein curvature.

Something sounds fishy to me here. I don't think this is true. As the star collapses the gravitational potential energy of the matter decreases. The volume decreases as well. So while the pressure increases and the energy density increases the volume decreases (less matter to integrate over) and the gravitational potential energy decreases. Thus the gravitational field at a set distance would seem to remain unchanged.

I'm not sure how you are defining "gravitational potential energy", but I think I agree with your conclusion if not the steps you take to reach it.

If an observer at infinity in flat space-time looks at the gravitational field of a collapsing star, he won't see any change in the "gravitational force", and the total mass of the star won't change, either. Well, I have to qualify that a bit - there's some possibiity that gravitational waves could carry away some energy, also the emission of light / electromagnetic radiation from the collapsing star could also carry away some energy. Other than losses due to radiation, the distant observer won't see any change in the "gravitational force" or the total mass as the star collapses.

From the point of view of preventing collapse, though (which was what the original question is about), the energy per unit volume is going up, and the pressure is going up as well, and both of these promote further collapse.

The fact that pressure causes gravity is one of the big differences between Einstein's theory and Newton's. This is what makes collapse to a singularity unstoppable in Einstein's theory. The pressure needed to resist collapse simply increases the field, overcoming the pressure, no matter how large the pressure gets. Not that by "field" here I'm not talking about the field as measured by a distant observer, which we both agree remains constant, but the Einstein curvature tensor - or the "thing that makes the ball of coffe grounds shrink" from Baez's GR tutorial.http://math.ucr.edu/home/baez/gr/outline2.html

The only thing then that can stop a singularity forming is if the force
gets smaller or stays constant.This happens for the colour force as quarks get closer together, so gravity might have something in common with it.

there's some possibiity that gravitational waves could carry away some energy, etc

Look up Birchoff's theorem. It implies that any body which is spherically symmeteric anc collapses in a spherical manner then the metric will remain the same outside the matter. And such a body does not radiate gravitational waves.

Interesting, but I had the impression that people are or will be looking (when LIGO comes online) for the gravitational waves emitted by collapsing stars. I believe the culprit here (as far as getting around Birkhoff's theorem) is the rotation of the star, though I'm not positive.

One example of a promising source of gravitational waves is the gravitational collapse of the rapidly rotating core of a massive star to a neutron star and the subsequent explosion of the star in a spectacular supernova event: Within fractions of a second a mass larger than that of our sun is compressed during the collapse to densities exceeding 100 millions of tons per cubic centimetre. The gravitational-wave signals produced typically consist of a strong short burst with a complicated temporal structure, and they depend crucially on many aspects of the complicated physics involved in this powerful event.

Interesting, but I had the impression that people are or will be looking (when LIGO comes online) for the gravitational waves emitted by collapsing stars. I believe the culprit here (as far as getting around Birkhoff's theorem) is the rotation of the star, though I'm not positive.

I don't know. But if a collapsing star collapses symmetrically and is symmetric to begin with then the gravitational radiation would be monopole radiation and in GR there is no monopole radiation.

I have more time to quote Rindler now

Birchoff's theorem has significant implications. Suppose, for example, the central spherical body were to start pulsating or exploding or imploding in a spherically symmetric (radial) way; the external field would show no trace of a response (Just as in Newton's theory!) In particular, no spherically symmetric gravitational radiation (being a progressive disturbance of the vacuum field) is possible.

Okay. Off I go to the butcher's block. :surprised See you if I make it out in one piece! :rofl:

In the real world, massive stars with iron cores which undergo collapse do so somewhat asymmetrically ... indeed, IIRC it wasn't until 2D (or was it 3D?) models were done that the core could collapse at all! In 1D (and maybe 2D?), the collapse stalls, no BH forms, etc. Apparently it's the tiny instabilities - deviations from perfect spherical symmetry? - which allow the collapse to proceed, somewhat like why water from an upturned bucket doesn't fall as a perfectly flat sheet?

The net result is that a core collapse SN *always* generates gravitational waves, because it does not (and cannot) collapse in a perfectly symmetrical fashion.

But is a rotating star "spherically symmetrical" in the sense of Birkhoff's theorem?

Wald says wrt Birkhoff's theorem

But of course we have the Kerr solution not equal to the Schwarzschild solution. The rotation spoils the spherical symmetry.

I doubt that there'd be a measurable effect. You're talking about an extremely small deviation from the Schwarzschild spacetime so any changes in the gravitational field would be extremly hard to even measure.